More Electron Traps — Question 3

Section 39-5 · Physics pages 6496–6497

Question 3 The harmonic position operator permits only neighboring-level dipole transitions A one-dimensional harmonic trap has V (x) = mω2x2/2 and En = (n + 1/2)ℏω, n = 0, 1, 2, . . .. Use x = √ ℏ/(2mω)(a + a†), a|n⟩= √n|n −1⟩and a†|n⟩= √n + 1|n + 1⟩. A weak electric field couples linearly to x. n = 0 n = 1 n = 2 E Schematic; labels, not drawing lengths, specify the data. (a) Derive ⟨r|x|n⟩and identify the allowed index changes. (b) Compare |x21|2 with |x10|2 and assess a direct 0 →2 electric-dipole transition.
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Question 3 - Solution The harmonic position operator permits only neighboring-level dipole transitions n = 0 n = 1 n = 2 E (a) Method and calculation ⟨r|x|n⟩= √ ℏ 2mω (√n δr,n−1 + √ n + 1 δr,n+1 ) . ∆n = ±1 for nonzero position matrix elements. (b) Interpretation and further calculation |x21|2/|x10|2 = 2 . x20 = 0 ⇒0 →2 absent in first-order dipole coupling . Physical check The ratio compares matrix-element strengths, not automatically total transition rates in different radiation environments. Multiphoton or nonlinear coupling is outside this model.

Question 3

The harmonic position operator permits only neighboring-level dipole transitions

A one-dimensional harmonic trap has V(x)=mω2x2/2V(x)=m\omega^2x^2/2 and En=(n+1/2)ℏωE_n=(n+1/2)\hbar\omega, n=0,1,2,…n=0,1,2,\ldots. Use x=ℏ/(2mω)(a+a†)x=\sqrt{\hbar/(2m\omega)}(a+a^\dagger), a|n⟩=n|n−1⟩a|n\rangle=\sqrt n|n-1\rangle and a†|n⟩=n+1|n+1⟩a^\dagger|n\rangle=\sqrt{n+1}|n+1\rangle. A weak electric field couples linearly to x.

Diagram shown in the original SVG worksheet.

  1. Derive ⟨r|x|n⟩\langle r|x|n\rangle and identify the allowed index changes.

  2. Compare |x21|2|x_{21}|^2 with |x10|2|x_{10}|^2 and assess a direct 0→20\to2 electric-dipole transition.

Question 3 - Solution

The harmonic position operator permits only neighboring-level dipole transitions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨r|x|n⟩=ℏ2mω(nδr,n−1+n+1δr,n+1).\langle r|x|n\rangle=\sqrt{\frac{\hbar}{2m\omega}}\left(\sqrt n\,\delta_{r,n-1}+\sqrt{n+1}\,\delta_{r,n+1}\right).Δn=±1for nonzero position matrix elements.\boxed{\Delta n=\pm1}\quad\text{for nonzero position matrix elements}.

(b) Interpretation and further calculation

|x21|2/|x10|2=2.\boxed{|x_{21}|^2/|x_{10}|^2=2}.x20=0⇒0→2 absent in first-order dipole coupling.\boxed{x_{20}=0}\Rightarrow\boxed{0\to2\text{ absent in first-order dipole coupling}}.

Physical check

The ratio compares matrix-element strengths, not automatically total transition rates in different radiation environments. Multiphoton or nonlinear coupling is outside this model.